JP2005311679A - Piezoelectric vibrating element - Google Patents

Piezoelectric vibrating element Download PDF

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JP2005311679A
JP2005311679A JP2004125571A JP2004125571A JP2005311679A JP 2005311679 A JP2005311679 A JP 2005311679A JP 2004125571 A JP2004125571 A JP 2004125571A JP 2004125571 A JP2004125571 A JP 2004125571A JP 2005311679 A JP2005311679 A JP 2005311679A
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piezoelectric
frequency
piezoelectric element
shape
circumscribed circle
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Yasuo Omori
靖男 大森
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OYO DENSHI KENKYUSHO KK
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OYO DENSHI KENKYUSHO KK
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a piezoelectric vibrating element independently generating a sound pressure characteristic and a frequency characteristic required in the market, such as a wideband and flat sound characteristic, as a result of reduction of a peak and a dip in a frequency graph produced by a polygonal piezoelectric element having a circular shape and a circumscribed circle. <P>SOLUTION: By generating the piezoelectric vibrating element including the polygonal piezoelectric element having no circumscribed circle and a vibrating plate, the distance from the center point of the piezoelectric vibrating element to circumference comes to variety. As a result, a sound pressure difference of the peak and the dip in the frequency graph becomes small, and thus wideband and nearly flat frequency characteristics are obtained. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

本発明は、振動板および圧電素子を用いた圧電振動素子に関する。 The present invention relates to a piezoelectric vibration element using a diaphragm and a piezoelectric element.

圧電素子を金属板あるいは樹脂などの振動板に貼り付けた圧電振動素子は、小型かつ軽量であるという特徴から、マグネットに変わりスピーカやレシーバ、マイクなどの材料として電子機器や携帯機器類などに搭載され始めており、そこに使用されている圧電素子の形状は円形または長方形など外接円を持つ多角形がほとんどである。   Piezoelectric vibration elements with a piezoelectric element attached to a vibration plate such as a metal plate or resin are mounted on electronic devices and portable devices as materials for speakers, receivers, microphones, etc. instead of magnets due to their small size and light weight. The shape of the piezoelectric element used therein is almost a polygon having a circumscribed circle such as a circle or a rectangle.

ただし従来のような形状の圧電素子では、再生音質の低下や低い周波数帯域の音が再生困難であるといった理由から、電極の形状を圧電素子の形状と変えたり(例えば、特許文献1参照)、振動板の形状を圧電素子の形状と変えて分割させたり(例えば、特許文献2参照)することによって、音響特性の向上を図るための発明がなされている。
特願平8−019095号公開特許公報 特願2001−016692号公開特許公報
However, in the case of a piezoelectric element having a conventional shape, the shape of the electrode may be changed to the shape of the piezoelectric element because the reproduction sound quality deteriorates and it is difficult to reproduce sound in a low frequency band (for example, see Patent Document 1). An invention has been made to improve acoustic characteristics by changing the shape of the diaphragm from the shape of the piezoelectric element and dividing it (see, for example, Patent Document 2).
Japanese Patent Application No. 8-019095 Japanese Patent Application No. 2001-016692

しかしながら、以上のような先行技術においても圧電素子そのものの形状は従来と変わらないため、圧電素子自体が有する周波数特性は変わらない。即ち、円形の圧電素子の場合は円形内部の中心点から周縁までの振動エネルギーの到達距離が半径であり、距離が一定であるため、振動エネルギーの複合として現れる周波数特性のグラフにおいて、ある一定の周波数帯域に一つのピークを持つという特徴が現れる。従って、円形の圧電素子を使用する場合は警報ブザーなど、音圧の大きな一つのピークを持つことが優位になるアプリケーションに使用されているのである。   However, in the prior art as described above, since the shape of the piezoelectric element itself is not different from the conventional one, the frequency characteristics of the piezoelectric element itself are not changed. That is, in the case of a circular piezoelectric element, since the arrival distance of vibration energy from the center point to the periphery inside the circle is a radius and the distance is constant, in the graph of frequency characteristics that appears as a composite of vibration energy, a certain constant The feature of having one peak in the frequency band appears. Therefore, when a circular piezoelectric element is used, it is used for an application where it is advantageous to have one peak with a large sound pressure, such as an alarm buzzer.

また長方形など外接円を持つ多角形の圧電素子の場合は、中心点から周縁までの距離が一定では無いため、距離の違いに応じて複合される振動エネルギーも円形に比べて多様になるが、中心点から周縁までの距離は外接円の半径に近いため、周波数特性のグラフにおいてもいくつかの周波数帯域に音圧のピークとディップが生じることになる。 Also, in the case of polygonal piezoelectric elements with circumscribed circles such as rectangles, the distance from the center point to the periphery is not constant, so the vibration energy combined according to the difference in distance is more diverse than the circle, Since the distance from the center point to the peripheral edge is close to the radius of the circumscribed circle, sound pressure peaks and dips occur in several frequency bands even in the graph of frequency characteristics.

以上のことから、円形および外接円を持つ多角形の圧電素子の場合は、一つまたは複数の音圧のピークおよびディップが生じ、その結果として再生音質が悪く、特にスピーカとして利用される際に要求される広帯域でかつフラットな音響特性が得られない。   From the above, in the case of a polygonal piezoelectric element having a circular shape and a circumscribed circle, one or a plurality of sound pressure peaks and dips occur, resulting in poor reproduction sound quality, particularly when used as a speaker. The required broadband and flat acoustic characteristics cannot be obtained.

また、先行技術のように音質の向上を図るために周辺部位の形状や筐体構造を工夫することは歩留まり、手間やコストの問題など新たな製作上の課題を生じることになる。   In addition, in order to improve sound quality as in the prior art, devising the shape of the peripheral part and the housing structure leads to new production problems such as yield and labor and cost.

本発明はこのような事情に鑑みてなされたものであり、円形および外接円を持つ多角形の圧電素子から生じる周波数グラフのピークやディップを軽減し、その結果それ単独で広帯域かつフラットな音響特性など市場で要求のある音圧や周波数特性を発生させることができる圧電振動素子を提供することを課題とする。   The present invention has been made in view of such circumstances, and reduces the peak and dip of the frequency graph generated from a polygonal piezoelectric element having a circular shape and a circumscribed circle. It is an object of the present invention to provide a piezoelectric vibration element that can generate sound pressure and frequency characteristics required in the market.

本発明では、外接円を持たない多角形であり、少なくとも対向する2つ以上の角を持ち
、角と角の間が曲線で結ばれている形状をなす振動板に同一形状の圧電素子を貼り付けた圧電振動素子を提供することで上記課題を解決する。
In the present invention, a piezoelectric element having the same shape is attached to a vibration plate having a shape that is a polygon that does not have a circumscribed circle, has at least two opposing corners, and the corners are connected by curves. The above-described problems are solved by providing the attached piezoelectric vibration element.

本発明は、外接円を持たない多角形である振動板に同一形状の圧電素子を貼り付けた圧電振動素子を提供することにより、従来の円形や外接円を持つ多角形の圧電素子に比べて中心点と周縁の距離の違いにより生ずる複合された振動エネルギーの種類が多く、その結果として広帯域にわたってフラットな音響特性を得ることができる。また以上の音響特性は圧電振動素子単独で実現することができるため、周辺部位や筐体構造の工夫も不要になる。   The present invention provides a piezoelectric vibration element in which a piezoelectric element having the same shape is attached to a polygonal diaphragm having no circumscribed circle, thereby making it possible to compare the conventional piezoelectric element with a circular or circumscribed circle. There are many types of combined vibration energy caused by the difference in the distance between the center point and the periphery, and as a result, flat acoustic characteristics can be obtained over a wide band. In addition, since the above acoustic characteristics can be realized by the piezoelectric vibration element alone, it is not necessary to devise peripheral parts or a housing structure.

本発明の圧電振動素子を利用したスピーカを製作した場合とその音響特性を、従来の形状の圧電素子を利用したスピーカの場合と比較することにより発明を実施するための最良の形態を示す。   The best mode for carrying out the invention is shown by comparing the case where a speaker using the piezoelectric vibration element of the present invention is manufactured and the acoustic characteristics thereof with the case of a speaker using a piezoelectric element having a conventional shape.

図1は、従来の圧電素子を使用したスピーカであり、長方形の圧電素子1をそれと同一形状かつより大きな面積を有する振動板2に貼り付けた圧電振動素子5が樹脂3の上に接着剤で接着され、樹脂3の外縁は枠4で固定されている。尚この時、振動板2と枠4は接点を有していない。   FIG. 1 shows a speaker using a conventional piezoelectric element. A piezoelectric vibration element 5 in which a rectangular piezoelectric element 1 is bonded to a diaphragm 2 having the same shape and a larger area is bonded on a resin 3 with an adhesive. The outer edge of the resin 3 is fixed by a frame 4. At this time, the diaphragm 2 and the frame 4 have no contact.

図1のスピーカにおいて、圧電振動素子からそれぞれプラスとマイナス電極を取り出し、アンプおよび音源に接続させる(アンプ、音源は図示せず)。アンプおよび音源を通じて圧電振動素子に音声信号が入力されると、圧電振動素子が振動することにより、音声が再生される。 In the speaker of FIG. 1, the positive and negative electrodes are respectively taken out from the piezoelectric vibration element 5 and connected to an amplifier and a sound source (the amplifier and the sound source are not shown). When an audio signal is input to the piezoelectric vibration element 5 through an amplifier and a sound source, the piezoelectric vibration element 5 vibrates to reproduce sound.

圧電振動素子に6Vの電圧を入力し、マイクから10cm離れた位置で再生された音声を測定した時の周波数特性を表したのが図2のグラフになる。グラフの縦軸は音圧を表し、75dBの場合を基準値にして上限が95dB、下限が55dBになっている。またグラフの横軸は周波数を表し、周波数帯の範囲は20Hzから20KHzになっている。図2を見てわかるように、従来の長方形の圧電素子1を用いたスピーカにおける周波数特性は、複数の大きなピークと大きなディップを有するため再生音質が均一ではなく、特に5KHz周辺および10KHz周辺の周波数の音声が突出して聞こえることになる。 The graph of FIG. 2 shows the frequency characteristics when a voltage of 6 V is input to the piezoelectric vibration element 5 and the sound reproduced at a position 10 cm away from the microphone is measured. The vertical axis of the graph represents the sound pressure, and the upper limit is 95 dB and the lower limit is 55 dB with a reference value of 75 dB. The horizontal axis of the graph represents frequency, and the frequency band range is 20 Hz to 20 KHz. As can be seen from FIG. 2, the frequency characteristics of the speaker using the conventional rectangular piezoelectric element 1 have a plurality of large peaks and large dips, so that the reproduced sound quality is not uniform, and particularly the frequencies around 5 KHz and 10 KHz. Will be heard in a protruding manner.

図3は、本発明の圧電振動素子を使用したスピーカであり、外接円を持たない多角形の圧電素子1をそれと同一形状かつより大きな面積を有する振動板2に貼り付けた圧電振動素子が樹脂3の上に接着され、樹脂3の外縁は枠4で固定されている。尚この時、振動板2と枠4は接点を有していない。
また図4は、図1における圧電振動素子のみを抽出した図である。
Figure 3 is a speaker using a piezoelectric vibrating element of the present invention, the piezoelectric vibrating elements 5 pasted to the vibration plate 2 having the identical shape and a larger area of the piezoelectric element 1 of the polygon that does not have a circumscribed circle It is bonded onto the resin 3 and the outer edge of the resin 3 is fixed by a frame 4. At this time, the diaphragm 2 and the frame 4 have no contact.
FIG. 4 is a diagram in which only the piezoelectric vibration element 5 in FIG. 1 is extracted.

図3のスピーカにおいても図1のスピーカと同様に、圧電振動素子からそれぞれプラスとマイナス電極を取り出し、アンプおよび音源に接続させる(アンプ、音源は図示せず
)。アンプおよび音源を通じて圧電振動素子に音声信号が入力されると、圧電振動素子
が振動することにより、音声が再生される。
In the speaker of FIG. 3, similarly to the speaker of FIG. 1, the plus and minus electrodes are taken out from the piezoelectric vibration element 5 and connected to an amplifier and a sound source (the amplifier and the sound source are not shown). When an audio signal is input to the piezoelectric vibration element 5 through an amplifier and a sound source,
When 5 vibrates, sound is reproduced.

この時図3の圧電振動素子に6Vの電圧を入力し、マイクから10cm離れた位置で再生された音声を測定した時の周波数特性を表したのが図5のグラフになる。グラフの縦軸および横軸の数値のとり方は、図2のグラフと同じである。図5を見てわかるように、本発明の圧電振動素子を利用したスピーカの場合は、図2と比べて250Hz以上の周波数帯においてはピークとディップの音圧の差が小さくなっているため、全体的に見てより広帯域でフラットに近い周波数特性が得られている。 At this time, the graph of FIG. 5 shows frequency characteristics when a voltage of 6 V is input to the piezoelectric vibration element 5 of FIG. 3 and the sound reproduced at a position 10 cm away from the microphone is measured. The method of taking the numerical values on the vertical and horizontal axes of the graph is the same as that of the graph of FIG. As can be seen from FIG. 5, in the case of the speaker using the piezoelectric vibration element of the present invention, the difference in the sound pressure between the peak and the dip is smaller in the frequency band of 250 Hz or higher than in FIG. Overall, frequency characteristics close to flat with a wider band are obtained.

以上のように本発明の圧電振動素子を用いることにより、従来の形状の圧電素子より広帯域でフラットに近い周波数特性が得られるが、その理由は圧電素子の中心点から周縁までの距離の違いにより生じる振動エネルギーが、本発明の圧電振動素子の方が多種類発生することで周波数特性グラフのピークやディップが補正されるからである。   As described above, by using the piezoelectric vibration element of the present invention, a frequency characteristic close to flat can be obtained in a wider band than the piezoelectric element of the conventional shape, because of the difference in distance from the center point of the piezoelectric element to the periphery. This is because the generated vibration energy is generated more in the piezoelectric vibration element of the present invention, so that the peak and dip of the frequency characteristic graph are corrected.

実施例では図4のように外接円を持たない八角形の圧電振動素子を用いて実験したが、この形状に限らず、レモンの形状のように少なくとも対向する2つ以上の角を持ち、角と角の間を曲線で結んだ形状外接円を持たない多角形であっても圧電素子の中心点から周縁までの距離が多様になるため、図4と同様に図5のような広帯域でフラットに近い周波数特性を得ることができる。   In the example, an experiment was performed using an octagonal piezoelectric vibration element having no circumscribed circle as shown in FIG. 4. However, the present invention is not limited to this shape, and has at least two opposing corners such as a lemon shape. Since the distance from the center point to the periphery of the piezoelectric element varies even if it is a polygon that does not have a circumscribed circle with a curved line between the corners and the corners, it is flat with a broadband as shown in FIG. A frequency characteristic close to can be obtained.

図1は、従来の形状の圧電素子を使用したスピーカの図である。FIG. 1 is a diagram of a speaker using a piezoelectric element having a conventional shape. 図2は図1のスピーカを用いた時に得られた音圧および周波数特性を示したグラフである。FIG. 2 is a graph showing sound pressure and frequency characteristics obtained when the speaker of FIG. 1 is used. 図3は本発明の圧電振動素子を使用したスピーカの図である。FIG. 3 is a diagram of a speaker using the piezoelectric vibration element of the present invention. 図4は本発明の圧電振動素子の一形状を示す図である。FIG. 4 is a view showing one shape of the piezoelectric vibration element of the present invention. 図5は図3のスピーカを用いた時に得られた音圧および周波数特性を示したグラフである。FIG. 5 is a graph showing sound pressure and frequency characteristics obtained when the speaker of FIG. 3 is used.

符号の説明Explanation of symbols

1 圧電素子
2 振動板
3 樹脂
4 枠
圧電振動素子
1 Piezoelectric element 2 Diaphragm 3 Resin 4 Frame
5 Piezoelectric vibration element

Claims (2)

振動板の片面あるいは両面に圧電素子を貼り付けた圧電振動素子であり、前記振動板は前記圧電素子と同一形状であり、圧電素子と同じ面積もしくは圧電素子より大きな面積を有する外接円を持たない多角形であることを特徴とした圧電振動素子。 A piezoelectric vibration element in which a piezoelectric element is attached to one or both surfaces of a vibration plate, and the vibration plate has the same shape as the piezoelectric element and does not have a circumscribed circle having the same area as the piezoelectric element or an area larger than the piezoelectric element. A piezoelectric vibration element characterized by being a polygon. 前記圧電振動素子は少なくとも対向する2つ以上の角を持ち、角と角の間を曲線で結んだ形状であることを特徴とした請求項1記載の圧電振動素子。 2. The piezoelectric vibration element according to claim 1, wherein the piezoelectric vibration element has a shape having at least two opposing corners and connecting the corners with a curve.
JP2004125571A 2004-04-21 2004-04-21 Piezoelectric vibrating element Pending JP2005311679A (en)

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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008080977A (en) * 2006-09-28 2008-04-10 Shin Kobe Electric Mach Co Ltd Battery state detection device and lead-acid battery for automobile
WO2013021906A1 (en) * 2011-08-08 2013-02-14 北陸電気工業株式会社 Piezoelectric sound element
WO2015008794A1 (en) * 2013-07-18 2015-01-22 北陸電気工業株式会社 Piezoelectric sound element

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008080977A (en) * 2006-09-28 2008-04-10 Shin Kobe Electric Mach Co Ltd Battery state detection device and lead-acid battery for automobile
WO2013021906A1 (en) * 2011-08-08 2013-02-14 北陸電気工業株式会社 Piezoelectric sound element
KR20140050655A (en) 2011-08-08 2014-04-29 호쿠리쿠 덴키 고교 가부시키가이샤 Piezoelectric sound element
JPWO2013021906A1 (en) * 2011-08-08 2015-03-05 北陸電気工業株式会社 Piezoelectric sounding element
US9398377B2 (en) 2011-08-08 2016-07-19 Hokuriku Electric Industry Co., Ltd. Piezoelectric sound element
WO2015008794A1 (en) * 2013-07-18 2015-01-22 北陸電気工業株式会社 Piezoelectric sound element
JPWO2015008794A1 (en) * 2013-07-18 2017-03-02 北陸電気工業株式会社 Piezoelectric sounding element

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